Understanding Raman Mode Representation at Specific Wave Numbers

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In summary, Raman modes are representations of the symmetry of the vibration being exited. For crystalline materials, there are a number of Raman active modes at particular wave numbers. The mode at 546 cm-1 can be written in place of 624 cm-1, but the mode at 624 cm-1 cannot be written in place of 546 cm-1. The mode at 546 cm-1 can be worked out experimentally from the polarisation and intensity of the incident and scattered light.
  • #1
sajid husain
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Why we describe Raman modes At perticular wave number by E1 or A1,A2 or other
If E1 say at 645cm-1, Why we cannot describe A1 at this wave number.
How we write the representation at perticlar wave number. Please reply.
 
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  • #2
These labels refer to the representation of the molecular point group.

The vibrational ground state always transforms as A1 and the excited state with one vibrational quantum transforms as some representation of the molecular symmetry group, e.g. E1. Then the excitation of one quantum of this vibration corresponds to an energy difference
##\Delta E=E_\mathrm{E1}-E_\mathrm{A1}=hc \tilde{\nu} ## where ##\tilde{\nu}## is the wavenumber of the Raman transition.
 
  • #3
Actually i am discussing about the space group symmetry of crystalline material how this mode assign for this name i.e, E1,A1, at particular wave number. Why these mods name come and what terminology behind this.Please clarify
 
  • #4
In crystalline media, the labels refer to the representation of the little group pertaining to the wavevector k. In Raman spectroscopy k=0, and that little group is identical to the crystallographic point group. The labels of the irreducible representations depend on the point group and are standardized. You have to look them up. For example A is a one-dimensional representation, E two dimensional and T three dimensional.
In Raman spectroscopy they refer to the symmetry of the vibration being exited. One quantum of vibration has a fixed energy, hence the asignment of a symmetry label to a wavelength.
 
  • #5
Ok Sir i agree with you...But For my System Aluminium Nitride There Are Number of mode in which A1,E1,E2 are raman active and E1 at 624 cm-1 and A1 546 cm-1, Why E1 cannot written at the place of 546 and A1 at 624?
 
  • #6
I think the representation can be worked out experimentally from the polarisation and intensity of the incident and scattered light.
For details you should have a look at some book on IR and Raman spectroscopy.
 

1. Why are A1, E1, E2, and B1 considered Raman modes?

The naming convention for Raman modes is based on the point group symmetry of a molecule. A1, E1, E2, and B1 are the four irreducible representations of a molecule's point group, and each represents a specific type of vibration or movement within the molecule. Thus, these modes are labeled as Raman modes.

2. What are the characteristics of A1, E1, E2, and B1 Raman modes?

A1 Raman modes are symmetric with respect to the center of inversion, E1 modes are asymmetric with respect to the center of inversion, E2 modes are doubly degenerate, and B1 modes are symmetric with respect to the mirror plane. These characteristics are determined by the molecule's point group and dictate the type of vibration or movement associated with each Raman mode.

3. How are A1, E1, E2, and B1 Raman modes observed?

Raman spectroscopy is the technique used to observe A1, E1, E2, and B1 Raman modes. This involves shining a laser onto a sample and measuring the scattered light. The scattered light contains information about the vibrational modes of the molecule, including the A1, E1, E2, and B1 modes.

4. What information can be obtained from A1, E1, E2, and B1 Raman modes?

The frequencies and intensities of A1, E1, E2, and B1 Raman modes provide information about the molecular structure and composition of a sample. This can include the types of bonds present, their lengths and strengths, and the overall symmetry of the molecule.

5. How do A1, E1, E2, and B1 Raman modes differ from IR-active modes?

A1, E1, E2, and B1 Raman modes are distinguishable from IR-active modes based on their selection rules. A1 and B1 Raman modes are only observed in polar molecules, while E1 and E2 modes can be observed in both polar and nonpolar molecules. Additionally, Raman modes involve changes in polarizability, while IR-active modes involve changes in dipole moment.

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